Superpotentials in IIA compactifications with general fluxes

By J. Derendinger, C. Kounnas, P. Petropoulos, F. Zwirner. 2004

278 citations recorded by the source corpus.

We derive the effective N = 1, D = 4 supergravity for the seven main moduli of type IIA orientifolds with D6 branes, compactified on T 6 /(Z2 × Z2) in the presence of general fluxes. We illustrate and apply a general method that relates the N = 1 �

Subfields: Astronomy and Astrophysics, Geometry and Topology, Nuclear and High Energy Physics

View Paper: https://www.semanticscholar.org/paper/c33d783950e233d59c33f0404344e095ef34376d

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The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.

In Astronomy and Astrophysics

1. Ralph Blumenhagen
2. Eran Palti
3. D. Lust
4. M. Graña
5. Gary Shiu
6. Thomas W. Grimm
7. M. Cvetič
8. Paul Koerber

In Geometry and Topology

1. M. Graña
2. Paul Koerber
3. Eran Palti
4. D. Lust
5. A. Tomasiello
6. M. Petrini
7. Gary Shiu
8. Ralph Blumenhagen

In Nuclear and High Energy Physics

1. D. Lust
2. Eran Palti
3. Ralph Blumenhagen
4. M. Graña
5. Gary Shiu
6. Thomas W. Grimm
7. M. Cvetič
8. Paul Koerber

Citations in the corpus

• The effective theory of type IIA AdS4 compactifications on nilmanifolds and cosets (2008, methodology): “The first examples of type IIA models where all the moduli were stabilized at tree level in a controlled classical supergravity regime were the torus orientifold models of [ 8 , 9, 10, 11].”
• Fluxes, moduli fixing and MSSM-like vacua in a simple IIA orientifold (2005, background): “settings one can also include metric fluxes and generate superpotential terms coupling both kinds of moduli [ 17 ,20].”
• Four-dimensional string compactifications with D-branes, orientifolds and fluxes (2006, background): “Only at the very end we briefly summarize advances towards the understanding of type IIA and heterotic flux vacua.”
• A ten-dimensional action for non-geometric fluxes (2011, background): “The latter is obtained by allowing, in addition to the usual fluxes in geometric situations [49, 50, 51, 52], the non-geometric fluxes as structure constants of the algebra.”
• De Sitter hunting in a classical landscape (2011, unknown): “The explicit forms of K, W , fαβ and Dα for the reduction of type IIA supergravity on SU(3)-structure spaces have been derived in many papers [37, 40–49] and the results are”
• Type IIA Moduli Stabilization (2005, unknown): “Departm entofPhysics Princeton University Princeton,NJ 08544,U.S.A. odewolfe@princeton.edu AlexanderGiryavets , Sham it Kachru Departm entofPhysicsand SLAC Stanford University Stanford,CA 94305/94309,U.S.A. giryav@stanford.edu, skachru@stanford.edu”
• T-duality and closed string non-commutative (doubled) geometry (2010, background): “We will give some evidence that for certain geometrical backgrounds, namely for geometric flux compactifications on twisted tori [19, 20, 21, 22, 23, 24, 25, 26], space with coordinates becomes non-commutative.”
• Generalized N=1 orientifold compactifications and the Hitchin functionals (2006, background): “Evidence for this identification is provided by comparing the generalized type IIA and type IIB superpotentials.”
• Generalized flux vacua (2006, unknown): “Our solutions do contain non-nilpotent algebras, however, (as do [32, 33]) and thus are in the class of vacua which seem most difficult to lift to ten dimensions.”
• TOWARD REALISTIC INTERSECTING D-BRANE MODELS (2005, background): “Alternatively, one can study directly Type IIA orientifolds with background fluxes (see [165] and references therein).”
• Gauged N=4 supergravities (2006, background): “Lower N theories can be obtained by truncation of the N = 4 supergravities, for example certain relevant N = 1 Kähler potentials can be computed from the N = 4 scalar potential [18, 19, 20].”
• Towards classical de Sitter solutions in string theory (2009, unknown): “[3, 35, 36]) for critical points.”
• The Swampland: Introduction and Review (2019, background): “Indeed, the general superpotential for a manifold with curvature that still has SU(3) structure was derived in [198,206–210] and reads”
• Duality Symmetric String and M-Theory (2013, background): “The theory of flux compactification on twisted tori is by now well developed [82, 79, 83, 84, 85, 86, 81, 87, 88, 89, 90] but lies outside the main thrust of this report (a helpful introduction can be found in the lectures of Wecht [91]).”
• More Dual Fluxes and Moduli Fixing (2006, background): “natural to incorporate metric fluxes [ 5 , 6] that correspond to generalized Scherk-Schwarz”
• A scan for new N = 1 vacua on twisted tori (2006, methodology): “This algebra was also obtained by Villadoro and Zwirner from a gauged supergravity analysis based on [3,4,8]: it realizes Scherk-Schwarz compactifications from 5 to 4 dimensions that break N = 4 to N = 2 (which becomes N = 1 after the orientifold), corresponding to a twist in the diagonal subgroup o”